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81.
应用比例积分控制原理将瞬态传热模型预测结果与出口 温度实测数据逐步进行反馈可准确预测原始静态地层温度. 为此, 本文基于井下各控制组件质量、动量及能量守恒原理, 建立了实际井身结构与钻具组合条件下循环和停止循环期间井筒-地层温度分布全瞬态传热模型, 应用全隐式有限差分法进行求解, 并引入比例积分控制原理对比分析实测温度与预测温度的误差范围进而精确、 快速获取原始地层温度. 结合一口深井基础数据计算表明, 套管下入深度改变了井筒-地层间热交换效率, 进而影响了近井壁地层温度分布状况; 同时, 钻井过程中循环和停止循环作业过程改变了井下各控制组件的初始条件与边界条件, 致使近井壁原始地层温度分布距离产生变化. 建立的数学模型和研究方法可为石油钻井、地热井开采及地球深部原始地层温度信息准确、 经济、快速获取提供理论基础.
关键词:
原始地层温度
循环与停止循环
瞬态传热模型
比例积分控制原理 相似文献
82.
For decades the research on thin-film growth has attracted considerable attention as these kinds of materials have the potential for a new generation of device application. It is known that the nuclei at the initial stage of the islands are more stable than others and certain atoms are inert while others are active. In this paper, by using kinetic Monte Carlo simulations, we will show that, when a surfactant layer is used to mediate the growth, a counter-intuitive fractal-to-compact island shape transition can be induced by increasing deposition flux or decreasing growth temperature. Specifically, we introduce a reaction-limited aggregation (RLA) theory, where the physical process controlling the island shape transition is the shielding effect of adatoms stuck to the stable islands on the incoming adatoms. Moreover, the origin of a transition from triangular to hexagonal and then to inverted triangular as well as the decay characteristics of three-dimensional islands on the surface and relations of our unique predictions with recent experiments will be discussed. Furthermore, we will present a novel idea to make use of the condensation energy of adatoms to control the island evolution along a special direction. 相似文献
83.
Yuki Yamamoto Jun‐ya Hasegawa Yoshikatsu Ito 《Journal of Physical Organic Chemistry》2012,25(3):239-247
The kinetics of carbamate formation from the reaction of carbon dioxide with α‐amino acids in D2O was first investigated by means of nuclear magnetic resonance spectroscopy. Potassium carbonate was used as the CO2 source. For each amino acid, the maximum carbamate yield, the apparent rate constant for the carbamate formation kapp, and the rate constants for the formation k1 and the breakdown k?1 of the carbamate were estimated. Plots of log k1 or log k?1 versus pKa of amino acids indicated that the formation rate k1 increased with the basicity (pKa) of amino acid, while the decomposition rate k?1 decreased. A Br?nsted β value of 0.39 was obtained from the former plot, being in good agreement with the previously reported ones (0.26–0.43). The observed negative pKa dependence of log k?1 (Br?nsted α = 0.34) is reasonable, because the carbamate decomposition is acid‐catalyzed and the steady‐state concentration of H+ should be higher for weaker basic amines. The charge (σ) and the lone‐pair energy (EN) at the nitrogen atom of the amino group were calculated. Although log k1 correlated with σ and EN, log k?1 was unrelated with both of these parameters. Considering that the carbamate formation (k1) is not only base‐catalyzed but should also be promoted by the nucleophilicity of the amino nitrogen, its correlation with σ and EN in addition to pKa is rational. The irrelevance of log k?1 to σ and EN is not surprising, because σ and EN are not a direct measure of [H+] of the solution. Copyright © 2011 John Wiley & Sons, Ltd. 相似文献
84.
V. Lepiller A. Goharzadeh A. Prigent I. Mutabazi 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,61(4):445-455
We have investigated the influence of a weak radial
temperature gradient in a wide gap and large aspect ratio
Couette-Taylor system. The inner cylinder is rotating and can be
heated or cooled, the outer cylinder is at rest and immersed in a
large thermal bath. We found that a radial temperature gradient
destabilizes the Couette flow leading to a pattern of traveling
helicoidal vortices occurring only near the bottom of the system.
The size of the pattern increases as the rotation frequency of the cylinder is increased. We
have characterized the spatiotemporal properties of the pattern and we have shown that it
behaves as a wall mode found in the simulation of the
complex Ginzburg-Landau equation with homogeneous boundary
conditions. 相似文献
85.
Nitridated /3-Ga2Os (100) substrate was investigated as the substrate for CaN epitaxial growth.The effects of nitridation temperature and surface roughness of -Ga2O3 wafers on the formation of CaN were studied. 相似文献
86.
Based on a review of the current literature, a surface phase diagram is proposed for the submonolayer Au on Si(111) system. Kinetic considerations are reviewed and key surface phase diagram features such as the Θ < 0.4 ML metastable
structure and the high temperature
to Si(111)-(1 × 1)Au second order phase transition are discussed. Experiments to verify certain portions of the phase diagram are proposed. 相似文献
87.
88.
从讨论波束形成方法在声系统中的主要作用和主要形成过程入手,介绍几种具体实现波束形成的算法。主要讨论一种能够降低硬件要求的波束形成算法——正交波束形成算法。此种方法不但适用于声系统,对于其他检测系统也有一定的实际意义。给出几种主要波束形成算法的Matlab仿真实现程序,将按照此类方法仿真所得到的波束形成指向性图与理论指向性图比较,两者非常类似。 相似文献
89.
利用溶胶-凝胶法成功制备了Mg掺杂Pb0.4Sr0.6MgxTi< sub>1-xO3-x薄膜,利用x射线衍射仪对薄膜的物相和结构进行了分析, 用扫描电子显微镜对薄膜的形貌和断面等进行了观察.研究结果表明,薄膜以立方钙钛矿为 晶相,薄膜中晶相以团聚状颗粒存在,晶相含量受热处理条件和Mg的掺杂量所控制.Mg掺杂 对Pb0.4Sr0.6MgxTi1-xO3-x 薄膜晶相含量的影响与钙钛矿中的氧空位缺陷相关.在一定的掺杂范围内,由掺杂引起晶相 的晶格畸变较小时,体系掺Mg平衡了晶体内本征氧空位引入的电荷不平衡,使晶相更为稳定 ,析晶能力提高,晶体形成量随掺杂浓度的提高而提高.当掺杂浓度达到一定量时, 随着Mg 掺杂浓度增加,一方面使形成晶体时杂质浓度增加造成参与形成晶相的组成含量下降,另一 方面使进入钙钛矿结构的Mg增加,氧空位大量增加使畸变程度提高,形成的晶相不稳定,析 晶能力下降,晶体含量随掺杂Mg浓度的增加而不增反降.在相同条件下制备的Pb0.4Sr0.6MgxTi1-xO3-x薄膜中Mg掺量约为 x=0.01时,得到的钙钛矿相含量最高,本征氧缺陷所带入的正电荷和Mg引入时带入的负电荷 间达到平衡.此外,Mg的掺入还影响到析晶与热处理过程之间的关系.在高Mg掺量范围,Mg含 量越高,形成的晶相越不稳定,热处理时间越长,使热处理过程中分解的晶相量越多,随Mg 掺量越高和热处理时间越长,薄膜中晶相含量越低.
关键词:
溶胶-凝胶法
PST薄膜
Mg掺杂
晶相形成 相似文献
90.
An attempt is made to synthesize Nd2Co14C compound by mechanical alloying Nd16Co76B8−xCx (0x8) alloys and subsequent annealing. Phase formation and magnetic properties of Nd2Fe14B-type Nd16Co76B8−xCx alloys and their hydrides are investigated. The Nd2Co14(B,C) phase with Nd2Fe14B-type structure is formed for Nd16Co76B8−xCx (0x7) alloys, while NdCo7Cδ phase with TbCu7-type structure is observed in Nd16Co76C8 alloy. The lattice parameter c of the Nd2Co14(B,C) phase decreases with increasing the carbon content. A limit volume of the unit cell to form the Nd2Fe14B-type structure is estimated to be 0.870 nm3. The spin-reorientation temperature TSR increases with increasing the carbon content, due to an enhancement of magnetocrystalline anisotropy caused by carbon substitution for boron. After hydrogenation, the lattice expansion is observed for Nd16Co76B8−xCx (0x7) alloys. The spin-reorientation temperature of Nd16Co76B8−xCxHy (0x7) is much lower than that of the host alloys. Some structural and magnetic properties of hypothetic Nd2Co14C and Nd2Co14CHy compounds are estimated by extrapolation. 相似文献